Research/Sitter/MAGNDATA / 0.171_DyScO3.mcif

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Spin lattice of DyScO3Spin lattice of DyScO3

DyScO3

MAGNDATA entry 0.171 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 3.2 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n ′m ′a ′ BNS 62.449
Parent space groupP n m a No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.669 · b 7.8515 · c 5.4136 Å · α 90° · β 90° · γ 90°
Transition3.15 K (−270 °C)
Measured at1.5 K
Magnetic ionsDy
Largest moment component8.36 μB
MethodNPD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P n ′m ′a ′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy00.2508.3604.449.4659
Sc1Sc000.5
O1O0.5550.250.8804
O2O0.3040.93920.6926

Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

L.S. Wu et al. PHYSICAL REVIEW B · doi:10.1103/PhysRevB.96.144407

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.171_DyScO3.mcif from MAGNDATA · entry page

sha256 of this copy: 3c93d7d4cd72b8104efdeca90dc5fc75890d4b054cf0acdd3dde772de56551d9
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.171_DyScO3.mcif.